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Table 13

Magnetic parameters of Ap stars with resolved magnetically split lines: stars with B data in this paper or in Paper I.

HD/HDE N m Bav σ B q N z Bzrms r N q Bqav p
(G) (G) (G) (G)

965 11 4315 30 1.08 7 982 7 7686
2453 14 3722 20 1.03 6 808 0.44 6 3962 1.16
9996 14 4717 30 1.34 63 713 0.35
12288 28 7978 120 1.11 20 1643 0.15
14437 32 7549 200 1.11 36 1930 0.35
18078 9 3508 120 1.81 25 692 0.92
29578 18 3085 40 1.53 9 785 9 3787
47103 7 17 321 50 1.06 6 2778 6 16 756
50169 21 5030 30 1.31 9 832 9 6431
51684 10 6027 50 1.09 7 1366 0.62 7 6605
55719 43 6465 60 1.13 12 719 12 7813
59435 19 3059 115 1.87
61468 15 6976 30 1.39 5 1884 0.23 5 6435 1.47
65339 30 12 770 900 1.95 19 3005 0.72
70331 38 12 416 300 1.10 16 2570 0.90 16 16 290
75445 16 2987 30 1.08 3 135 3 4275
81009 42 8382 115 1.23 13 1873 0.60 13 10356 1.13
93507 30 7146 110 1.09 12 2217 0.43 12 7679 1.43
94660 25 6183 30 1.06 12 1911 0.92 12 6880 1.53
110066 7 4088 30 1.03 3 117
116114 24 5960 25 1.01 7 1815 0.91 7 7646
116458 21 4677 30 1.00 21 1684 0.71 21 5549
119027 13 3166 100 1.22 1 510 1 3655
126515 22 12 417 120 1.69 19 1660 0.64 19 16 339 2.17
134214 30 3092 40 1.07 8 391 7 3977
137909 46 5476 45 1.09 21 604 0.64 21 6536
137949 20 4672 25 1.02 9 1629 9 4680
142070 24 4898 55 1.10 13 376 0.23 13 4733
144897 28 8992 170 1.13 13 1892 0.59 13 10 163 1.16
150562 12 4860 35 1.06 1 1206 1 5710
318107 36 14 192 300 1.22 6 2551 0.27 6 21 209
165474 37 6625 25 1.14 8 233 8 8349
166473 33 7126 80 1.45 10 1626 10 7923
177765 8 3415 20 1.02
187474 40 5423 25 1.27 20 1476 0.98 20 7128
188041 18 3653 25 1.02 9 1196 0.43
192678 35 4764 80 1.05 14 1451 0.81
335238 18 8678 300 1.54 3 1399 3 11 895
200311 35 8540 300 1.22 24 1410 0.99
201601 28 3881 35 1.10 18 1000 16 5241
208217 38 7872 350 1.27 8 961 0.46 8 10 273 1.24
213637 4 5189 50 1.05 1 230 1 5375
216018 23 5602 40 1.04 9 1381 9 6769

Notes. Each star is identified by its HD or HDE number. Nm is the number of measurements of the mean magnetic field modulus from which its average Bav is computed. For stars for which a full rotation cycle has not yet been observed, the latter appears in italics, as does the ratio q between the highest and lowest value of B. The σB is the estimated uncertainty of the B measurements (see Sect. 3.1 for details). Nz is the number of measurements from which the rms longitudinal field Bzrms is computed, and r is the ratio of the extrema of Bz (defined in Sect. 5.2); the value of r is given only for those stars for which Bz measurements have been obtained throughout a full rotation cycle. Values of Bzrms and r computed from mean longitudinal field measurements from the literature (rather than from this paper and from Paper I) appear in italics. Nq is the number of measurements of the mean quadratic field from which its average Bqav is computed; p is the ratio between the extrema of Bq, which is given only for stars for which Bq determinations have been obtained throughout a full rotation cycle.

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